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Space-time finite element methods for distributed optimal control of the wave equation

Published 4 Nov 2022 in math.NA, cs.NA, and math.OC | (2211.02562v1)

Abstract: We consider space-time tracking type distributed optimal control problems for the wave equation in the space-time domain Q:=Ω×(0,T)⊂R<sup>n+1Q:= \Omega \times (0,T) \subset {\mathbb{R}}<sup>{n+1}, where the control is assumed to be in the energy space [H0;,0<sup>1,1(Q)]<sup>∗[H_{0;,0}<sup>{1,1}(Q)]<sup>*, rather than in L<sup>2(Q)L<sup>2(Q) which is more common. While the latter ensures a unique state in the Sobolev space H<sup>1,10;0,(Q)H<sup>{1,1}_{0;0,}(Q), this does not define a solution isomorphism. Hence we use an appropriate state space XX such that the wave operator becomes an isomorphism from XX onto [H0;,0<sup>1,1(Q)]<sup>∗[H_{0;,0}<sup>{1,1}(Q)]<sup>*. Using space-time finite element spaces of piecewise linear continuous basis functions on completely unstructured but shape regular simplicial meshes, we derive a priori estimates for the error ∣u~<em>ϱh−u‾∣</em>L<sup>2(Q)|\widetilde{u}<em>{\varrho h}-\overline{u}|</em>{L<sup>2(Q)} between the computed space-time finite element solution u~ϱh\widetilde{u}_{\varrho h} and the target function u‾\overline{u} with respect to the regularization parameter ϱ\varrho, and the space-time finite element mesh-size hh, depending on the regularity of the desired state u‾\overline{u}. These estimates lead to the optimal choice ϱ=h<sup>2\varrho=h<sup>2 in order to define the regularization parameter ϱ\varrho for a given space-time finite element mesh size hh, or to determine the required mesh size hh when ϱ\varrho is a given constant representing the costs of the control. The theoretical results will be supported by numerical examples with targets of different regularities, including discontinuous targets. Furthermore, an adaptive space-time finite element scheme is proposed and numerically analyzed.

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